Academic literature on the topic 'Satellite orbital motion model'

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Journal articles on the topic "Satellite orbital motion model"

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Nakajima, Ayano, Shigeru Ida, and Yota Ishigaki. "Orbital evolution of Saturn’s satellites due to the interaction between the moons and the massive rings." Astronomy & Astrophysics 640 (August 2020): L15. http://dx.doi.org/10.1051/0004-6361/202038743.

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Context. Saturn’s mid-sized moons (satellites) have a puzzling orbital configuration with trapping in mean-motion resonances with every-other pairs (Mimas-Tethys 4:2 and Enceladus-Dione 2:1). To reproduce their current orbital configuration on the basis of a recent model of satellite formation from a hypothetical ancient massive ring, adjacent pairs must pass first-order mean-motion resonances without being trapped. Aims. The trapping could be avoided by fast orbital migration and/or excitation of the satellite’s eccentricity caused by gravitational interactions between the satellites and the rings (the disk), which are still unknown. In our research we investigate the satellite orbital evolution due to interactions with the disk through full N-body simulations. Methods. We performed global high-resolution N-body simulations of a self-gravitating particle disk interacting with a single satellite. We used N ∼ 105 particles for the disk. Gravitational forces of all the particles and their inelastic collisions are taken into account. Results. Dense short-wavelength wake structure is created by the disk self-gravity and a few global spiral arms are induced by the satellite. The self-gravity wakes regulate the orbital evolution of the satellite, which has been considered as a disk spreading mechanism, but not as a driver for the orbital evolution. Conclusions. The self-gravity wake torque to the satellite is so effective that the satellite migration is much faster than was predicted with the spiral arm torque. It provides a possible model to avoid the resonance capture of adjacent satellite pairs and establish the current orbital configuration of Saturn’s mid-sized satellites.
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Dubrovin, A. G., Yu N. Baranov, and A. P. Tryastsin. "The development of the model of satellite orbital motion." IOP Conference Series: Materials Science and Engineering 450 (December 4, 2018): 022033. http://dx.doi.org/10.1088/1757-899x/450/2/022033.

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Palkin, M. V., and I. P. Titkov. "Satellite Formation Flying Maneuver Control." Mekhatronika, Avtomatizatsiya, Upravlenie 20, no. 5 (2019): 308–13. http://dx.doi.org/10.17587/mau.20.308-313.

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A problem of a formation flying satellites maneuver control is presented. Among the most important criteria for satellite formation flying control system are active period maximization, precision of the configuration, secure motion (without collisions of satellites). Several methods for group configuration are presented: periodic impulse correction of each flying satellite position formation ("continuous order"); method of a satellite positioning on non-coplanar orbits ("variable order"). Other methods include combinations of methods mentioned above. Recommendations for their application are given. Two ideologies for satellite formation flying can be presented. The first one includes independent maintenance of each satellite a priori specified orbital parameters. The second one implies specialization of satellites: leaders provide orbital parameters for following satellites. Theory of the optimal control of multiobject multi-criteria systems is supposed to be rational for the maneuver control of a group of satellites. Based on this theory algorithm consists of the following phases. On the first phase current intergroup orbiting parameters are measured. On the second phase direction, capacity and duration of the control impulse are estimated based on the forecast of satellite orbital parameters and optimization criteria. On the last phase, the thrusters are used to issue a control impulse. In the presented paper such algorithm is adopted for a task of a formation flying control based on criterion, which consists of two parts. The first part is a configuration deformation minimization. The second one is a distance maximization near orbital node. Algorithm consists of three phases. On the first phase current intergroup orbiting parameters are measured. On the second phase orbital parameters in the "nodе" points are forecasted. On the third phase control parameters are estimated. A model example is given, computational complexity for different number of satellites is determined. Recommendations for practical application of the algorithm are given.
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MUNUSAMY, Raja, Kokila VASUDEVAN, and R. SUNDARAMOORTHY. "Design and Analysis of AAUSAT Cube Satellite Attitude Determination with PID Algorithms and Orbitron TLE." INCAS BULLETIN 15, no. 2 (2023): 49–57. http://dx.doi.org/10.13111/2066-8201.2023.15.2.5.

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Satellites are intended to be of massive cost, hard, or hard to keep up and fix in circle. The point of this task is to decide an effective strategy to decide the orbital and heading data for the Nano satellite. To design the exact trajectory and circle for a satellite, information regarding the components which are liable for the deviation in the method of satellites. The factors that should be taken into account to determine the exact location of the satellite. It could be accomplished with the assistance of software responsible for orbit simulation, to do programming with Orbitron so as to get the required output. Orbitron is a simple 2D solver in which TLE files are uploaded, for AAUSAT CUBESAT. The various impacts on the satellite in space are slight deviation in the satellite from its orbit. The motion of the body with includes the disturbing forces in the orbit. However, a satellite has deviated from its normal path due to several forces. This deviation is termed as orbital perturbation. The changes in the orbital element with respect to secular variations are considered using orbital quaternions. The output from satellite dynamic model is received from attitude sensor. The comparative data (Input and Feedback) will generate error signal. To minimize the error signal using proportional integral and derivative (PID) is proposed controller implemented with MATLAB environment.
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Shatina, A. V., M. I. Djioeva, and L. S. Osipova. "Mathematical Model of Satellite Rotation near Spin-Orbit Resonance 3:2." Nelineinaya Dinamika 18, no. 4 (2022): 0. http://dx.doi.org/10.20537/nd220803.

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This paper considers the rotational motion of a satellite equipped with flexible viscoelastic rods in an elliptic orbit. The satellite is modeled as a symmetric rigid body with a pair of flexible viscoelastic rods rigidly attached to it along the axis of symmetry. A planar case is studied, i. e., it is assumed that the satellite’s center of mass moves in a Keplerian elliptic orbit lying in a stationary plane and the satellite’s axis of rotation is orthogonal to this plane. When the rods are not deformed, the satellite’s principal central moments of inertia are equal to each other. The linear bending theory for thin inextensible rods is used to describe the deformations. The functionals of elastic and dissipative forces are introduced according to this model. The asymptotic method of motions separation is used to derive the equations of rotational motion reflecting the influence of the fluctuations, caused by the deformations of the rods. The method of motion separation is based on the assumption that the period of the autonomous oscillations of a point belonging to the rod is much smaller than the characteristic time of these oscillations’ decay, which, in its turn, is much smaller than the characteristic time of the system’s motion as a whole. That is why only the oscillations induced by the external and inertial forces are taken into account when deriving the equations of the rotational motion. The perturbed equations are described by a third-order system of ordinary differential equations in the dimensionless variable equal to the ratio of the satellite’s absolute value of angular velocity to the mean motion of the satellite’s center of mass, the angle between the satellite’s axis of symmetry and a fixed axis and the mean anomaly. The right-hand sides of the equation depend on the mean anomaly implicitly through the true anomaly. A new slow angular variable is introduced in order to perform the averaging for the perturbed system near the 3:2 resonance, and the averaging is
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Gorchakov, S. Yu. "Mathematical modeling of velocity and accelerations fields of image motion in the optical equipment of the Earth remote sensing satellite." Russian Technological Journal 11, no. 6 (2023): 47–56. http://dx.doi.org/10.32362/2500-316x-2023-11-6-47-56.

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Objectives. The paper considers a satellite with an optoelectronic payload designed to take pictures of the Earth’s surface. The work sets out to develop a mathematical model for determining the dependencies between the state vector of the satellite, the state vector of the point being imaged on the Earth’s surface, and the distribution fields of the velocity vectors and accelerations of the motion of the image along the focal plane of the optoelectronic payload.Methods. The method is based on double differentiation of the photogrammetry equation when applied to a survey of the Earth’s surface from space. For modeling the orbital and angular motion of the satellite, differential equations with numerical integration were used. The motion parameters of the Earth’s surface were calculated based on the Standards of Fundamental Astronomy software library.Results. Differential equations of motion of the image were obtained. Verification of the developed mathematical model was carried out. The motion of the considered satellite was simulated in orbital orientation mode using an image velocity compensation model. The distribution fields of velocity vectors and accelerations of motion of the image of the Earth’s surface were constructed. The residual motion of the field of image following compensation was investigated.Conclusions. The proposed mathematical model can be used both with an optoelectronic payload when modeling shooting modes and estimating image displacements at the design stage of a satellite, as well as at the satellite operation stage when incorporating the presented model in the onboard satellite software. The presented dependencies can also be used to construct an image transformation matrix, both when restoring an image and when obtaining a super-resolution.
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Yoon, Yihun, Woojae Jang, and Jintai Chung. "Natural Frequencies of a Tethered Satellite System." Applied Sciences 15, no. 4 (2025): 2180. https://doi.org/10.3390/app15042180.

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This study investigated the natural frequencies of a tethered satellite system to enhance stability and operational reliability. Tethered satellite systems provide many advantages for space missions but exhibit inherently complex dynamics due to the interaction between rigid-body motions and tether deformation. A dumbbell model was employed to analyze rigid-body dynamics, with eigenvalue analysis used to determine the natural frequencies of orbital and librational motion. Additionally, tether deformation was examined through simulations based on the absolute nodal coordinate formulation (ANCF) and a tensioned beam model, facilitating both analytical and computational assessments of transverse and longitudinal frequencies. The results show that orbital angular velocity and libration frequencies are highly sensitive to system parameters such as tether length, orbital radius, and satellite masses. Furthermore, the transverse and longitudinal natural frequencies of the tether exhibit distinct dependencies, providing critical insights for the design and control of tethered satellite systems. This work bridges a gap in understanding coupled dynamics and offers a systematic framework for calculating natural frequencies, supporting practical implementation in space missions.
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Kudryavtsev, Sergey M. "New semi-analytical calculation of lunar, solar and planetary perturbations in motion of Earth satellites." Proceedings of the International Astronomical Union 18, S382 (2022): 142–45. http://dx.doi.org/10.1017/s1743921323003988.

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AbstractWe suggest an advanced algorithm for semi-analytical calculation of orbital perturbations of Earth artificial satellites caused by the gravity attraction of the “3rd-bodies” (the Moon, the Sun, major planets). A new accurate analytical series for the relevant perturbation function is developed. It is obtained through a careful spectral analysis of the long-term DE406 planetary/lunar ephemerides and valid over 2000 years, 1000-3000. The series is used in the author’s semi-analytical model of satellite motion. The results of the motion prediction of several Earth satellites obtained by means of the semi-analytical model and a numerical integration method are compared.
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Chernikova, Oksana Sergeevna, and Yuliya Sergeevna Chetvertakova. "Two-stage parametric identification procedure to predict satellite orbital motion." International Journal of Electrical and Computer Engineering (IJECE) 12, no. 5 (2022): 5348. http://dx.doi.org/10.11591/ijece.v12i5.pp5348-5354.

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<span>The paper presents a new step-by-step procedure for constructing a navigation satellite motion model. At the first stage of the procedure, the parameters of the radiation pressure model are estimated using the maximum likelihood method. The statistic estimator based on the continuous-discrete adaptive unscented Kalman filter is proposed for the solar radiation model parameters estimation. Step-by-step scheme of filtering algorithm used for the software development are given. At the second stage, the parameters of the unaccounted perturbations model are estimated based on the results of residual differences measurements. The obtained results lead to significant improvement of prediction quality of the satellite trajectory.</span>
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Yakovlev, O. Ya, and D. V. Malygin. "External thermal modeling satellite platform «Synergy»." Spacecrafts & Technologies 3, no. 3 (2019): 155–63. http://dx.doi.org/10.26732/2618-7957-2019-3-155-163.

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In order to conduct thermal research of the satellite platform «Synergy», a mathematical model has been developed for calculating external thermal loads for spacecraft of the CubeSat form factor, operating in various orientation modes in near-Earth circular orbits. When modeling thermal conditions, heat fluxes from the Sun, the earth's flux and atmospheric effects are taken into account. A feature of the model is the transition to a moving geocentric coordinate system for determining the density of heat fluxes of direct and reflected solar radiation. The study of thermal conditions in the process of orbital motion is carried out and the parameters of the position of the orbital plane and the parameters of the Sun are determined at which the maximum and minimum average integral thermal loads are achieved during the orbital period. In these orbits, the motion of the satellite platform was simulated in three typical orientation modes and the density values of the absorbed heat fluxes by its external elements were determined. Four options for the design of the housing are being investigated. The data obtained during the simulation were used for the initial stationary calculation of the temperature field of the satellite platform in the ANSYS software package. The most interesting cases from the point of view of the thermal regime for further thermal research have been identified.
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Dissertations / Theses on the topic "Satellite orbital motion model"

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Snider, James Ralph. "Satellite motion around an oblate planet: a perturbation solution for all orbital parameters." Thesis, Monterey, California. Naval Postgraduate School, 1989. http://hdl.handle.net/10945/26751.

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Panzetta, Francesca. "Determination of the ocean tide model from LEO satellite orbital perturbation analysis." Doctoral thesis, Università degli studi di Padova, 2013. http://hdl.handle.net/11577/3423424.

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The present study concerns the determination of ocean tide model parameters from GOCE orbital perturbation analysis. The GOCE satellite was launched by the European Space Agency in 2009 and is flying on a Sun-synchronous near circular orbit, at the very low altitude of about 250 km which makes it very sensitive to tidally induced orbit perturbations. The strategy adopted for analyzing GOCE GPS tracking data is the direct fully-dynamic approach, consisting in the GOCE precise orbit determination (POD) and accumulation of the normal equations for each orbital arc, followed by a multiarc solution for the estimation of the global ocean tide parameters. The GOCE GPS observations are processed using the NAPEOS S/W system (ESA/ESOC), specific for satellite orbit determination and prediction, upgraded to inclusion of the partial derivatives with respect to the ocean tide parameters and the ocean tide model inversion capability. A sensitivity study of the ocean tide perturbations on GOCE orbit was carried out using as a reference the FES2004 model, in order to define the set of tidal harmonic parameters affecting GOCE orbit. In particular, the secular rates of the GOCE angular elements are estimated through a linear least-square fit. From GOCE mean orbital characteristics, the spectral analysis of ocean tide perturbations in the radial, transverse and normal direction is performed using Kaula's linear satellite theory. Then, the perturbation statistics by coefficient is computed, obtaining a maximum RMS of about 1.323 m for the radial component, 363.136 m for the transverse component and 76.241 m for the normal component. The temporal aliasing problem is also accounted for the recovery of tidal parameters with GOCE and the principal alias periods are calculated for each tidal perturbation frequency, considering the length of the available GOCE data record. To fix a limit for the number of parameters to be estimated, three different cutoffs are applied to the RMS perturbation coefficients, respectively equal to 5 mm for the radial component, 2 cm for the transverse component and 1 cm for the normal component, both in the prograde and retrograde case. The total parameters to be estimated result to be 490. GOCE data are processed to perform the fully-dynamic POD over daily orbital arcs from the 1st November 2009 until the 31st May 2011, but only arcs with a post-fit RMS of the GPS phase observations residuals lower than 8 mm are considered for the multiarc processing, for a total of 431 days. The obtained preliminary results show the relative error of the estimated parameters with respect to the corresponding FES2004 parameters lower than 1 for about the 16\% of the total, meaning that they are of the order of magnitude of the FES2004 parameters. GOCE orbital data were reprocessed along the same period of the previous run, initializing the ocean tide model with the estimated parameters, if present, and maintaining otherwise the FES2004 parameters. The post-fit RMS of the GPS phase residuals obtained with the new ocean tide model has a mean value of 6.5 mm, and it is noteworthy that the difference between the post-fit RMS obtained with the FES2004 model and that resulting from the new ocean tide model indicates a mean improvement of about 0.6 mm in for the 96\% of the analyzed arcs and greater than 1 mm for the 16\%, few days reach a difference of 2 mm. Finally, the orbits obtained with the estimated parameters are compared with the orbits obtained employing the FES2004 model and the official GOCE Reduced-Dynamic PSO. The 3D RMS of the difference between the orbits computed using FES2004 and those recomputed with the new parameters shows a mean value of 2.5 cm, while the 3D RMS of the difference with respect to the official R/D PSO has a mean value of 4.9 cm. Moreover, the difference between the 3D RMS of the orbit residuals between the R/D PSO and the GOCE POD with FES2004 and the RMS of the difference between the GOCE R/D PSO and the GOCE POD with the new parameters results to have a mean improvement of 0.9 cm. Further POD-Multiarc runs are certainly necessary, together with the refinement of the list of parameters to be estimated, removing excessively ill-estimated ocean tide parameters and introducing new parameters where appropriate. Indeed, the model parameter tuning and investigation is essential to adjust the best combination of parameters to be estimated. Moreover, an extension of the data set to much longer time-period should allow a substantial improvement of the obtained results. The task has proven very intensive and challenging, but the partial results obtained are encouraging and a motivation for future analysis.<br>Il presente lavoro di ricerca riguarda la determinazione dei parametri del modello di marea oceanica dall'analisi delle perturbazioni orbitali di GOCE. Il satellite GOCE è stato lanciato dall'Agenzia Spaziale Europea nel 2009 e volando a quota estremamente bassa, pari a circa 250 km, è molto sensibile alle perturbazioni orbitali indotte dalle maree. La strategia adottata per l'analisi dei dati GPS GOCE è l'approccio numerico diretto caratterizzato da un modello di forza completo, per questo detto completamente dinamico, che consiste nella determinazione orbitale precisa (POD) di GOCE con accumulo delle equazioni normali per ogni arco orbitale, seguiti da una soluzione multiarco per la stima dei parametri globali di marea oceanica. Le osservazioni GPS di GOCE vengono elaborate utilizzando il S/W NAPEOS (ESA/ESOC), specifico per la determinazione orbitale di satelliti e aggiornato per includere le derivate parziali rispetto ai parametri di marea e la struttura che permetta l'inversione del modello di marea. Uno studio di sensibilità delle perturbazioni mareali sull'orbita di GOCE è stato eseguito utilizzando come modello di riferimento il FES2004, al fine di definire la griglia di parametri di marea che influenzano maggiormente l'orbita di GOCE. In particolare, è stata seguita la seguente procedura. Prima di tutto, le variazioni secolari degli elementi angolari di GOCE (argomento di perigeo, longitudine del nodo ascendente, anomalia media) sono state stimate con un fit lineare ai minimi quadrati. Dalle caratteristiche orbitali medie di GOCE, è stata eseguita l'analisi spettrale delle perturbazioni di marea oceanica in direzione radiale, trasversale e normale, utilizzando la teoria lineare di Kaula. In seguito, è stata effettuata la statistica delle perturbazioni per coefficiente, ottenendo un RMS massimo di circa 1.323 m per la componente radiale, 363.136 m per la componente trasversale e 76.241 m per la componente normale. E' stato affrontato anche il problema di aliasing temporale di cui soffrono i parametri di marea che devono essere stimati con GOCE e per ogni frequenza di perturbazione mareale sono stati calcolati i periodi principali di aliasing; si è considerata infine la lunghezza del set di dati GOCE disponibili. E' stato inoltre necessario fissare un limite per il numero di parametri da stimare, tre soglie diverse sono state applicate all'RMS delle perturbazioni per coefficiente, rispettivamente pari a 5 mm per la componente radiale, 2 cm per la componente trasversale e 1 cm per la componente normale, sia nel caso progrado che retrogrado. In tal modo, i parametri totali da stimare risultano essere 490. I dati orbitali di GOCE sono stati analizzati per la stima della POD su archi orbitali giornalieri, coprendo un periodo che va dal 1 novembre 2009 al 31 maggio 2011, ma sono stati considerati per il multiarc solo i giorni con un post-fit RMS dei residui delle osservazioni di fase GPS inferiore a 8 mm, per un totale di 431 giorni. I risultati ottenuti sono preliminari e mostrano un errore relativo dei parametri stimati rispetto ai corrispondenti parametri del FES2004 inferiore a 1 per circa il 16% del totale, il che significa che sono dell'ordine di grandezza dei parametri del FES2004. I dati orbitali di GOCE sono stati poi rielaborati lungo lo stesso periodo di analisi, inizializzando il modello di marea oceanica con i nuovi parametri stimati, dove possibile, mantenendo altrimenti i parametri del FES2004. Il post-fit RMS dei residui di fase GPS ottenuti con il nuovo modello di marea ha un valore medio di 6.5 mm, ed è da notare che la differenza tra i post-fit RMS ottenuti con il FES2004 e quelli risultanti dal nuovo modello indicano un miglioramento medio di circa 0.6 mm per il 96% degli archi analizzati e maggiore di 1 mm per il 16%, mentre pochi giorni raggiungono una differenza di 2 mm. Infine, le orbite di GOCE ottenute con i parametri stimati vengono confrontate con le orbite ottenute usando il FES2004 e con le PSO ufficiali a dinamica ridotta. L'RMS 3D della differenza tra le orbite calcolate utilizzando il FES2004 e quelle calcolate con i nuovi parametri mostra un valore medio di 2.5 cm, mentre l'RMS 3D della differenza rispetto alle PSO a dinamica ridotta ha un valore medio di 4.9 cm. Inoltre, la differenza tra l'RMS 3D dei residui orbitali tra le PSO e la POD eseguita con il FES2004 e l'RMS 3D della differenza tra le PSO e la POD di GOCE eseguita con l'aggiunta dei parametri stimati mostra miglioramento medio di 0.9 cm. Ulteriori run di POD e multiarc sono certamente necessari, insieme alla rifinitura della lista dei parametri da stimare, rimuovendo quelli eccessivamente fuori dalla soluzione del FES2004 ed eventualmente introducendone opportunamente di nuovi. Infatti, è essenziale fare ulteriori e approfondite indagini per individuare la migliore combinazione di parametri di marea da stimare. Inoltre, l'estensione dei dati GOCE a un periodo di tempo più lungo dovrebbe consentire un sostanziale miglioramento dei risultati ottenuti. Il compito del presente lavoro di ricerca si è dimostrato molto intenso e impegnativo, ma i risultati parziali ottenuti sono incoraggianti e rappresentano una motivazione per le analisi future.
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Rogers, Andrew Charles. "Optimization-Based Guidance for Satellite Relative Motion." Diss., Virginia Tech, 2016. http://hdl.handle.net/10919/79455.

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Spacecraft relative motion modeling and control promises to enable or augment a wide range of missions for scientific research, military applications, and space situational awareness. This dissertation focuses on the development of novel, optimization-based, control design for some representative relative-motion-enabled missions. Spacecraft relative motion refers to two (or more) satellites in nearly identical orbits. We examine control design for relative configurations on the scale of meters (for the purposes of proximity operations) as well as on the scale of tens of kilometers (representative of science gathering missions). Realistic control design for satellites is limited by accurate modeling of the relative orbital perturbations as well as the highly constrained nature of most space systems. We present solutions to several types of optimal orbital maneuvers using a variety of different, realistic assumptions based on the maneuver objectives. Initially, we assume a perfectly circular orbit with a perfectly spherical Earth and analytically solve the under-actuated, minimum-energy, optimal transfer using techniques from optimal control and linear operator theory. The resulting open-loop control law is guaranteed to be a global optimum. Then, recognizing that very few, if any, orbits are truly circular, the optimal transfer problem is generalized to the elliptical linear and nonlinear systems which describe the relative motion. Solution of the minimum energy transfer for both the linear and nonlinear systems reveals that the resulting trajectories are nearly identical, implying that the nonlinearity has little effect on the relative motion. A continuous-time, nonlinear, sliding mode controller which tracks the linear trajectory in the presence of a higher fidelity orbit model shows that the closed-loop system is both asymptotically stable and robust to disturbances and un-modeled dynamics. Next, a novel method of computing discrete-time, multi-revolution, finite-thrust, fuel-optimal, relative orbit transfers near an elliptical, perturbed orbit is presented. The optimal control problem is based on the classical, continuous-time, fuel-optimization problem from calculus of variations, and we present the discrete-time analogue of this problem using a transcription-based method. The resulting linear program guarantees a global optimum in terms of fuel consumption, and we validate the results using classical impulsive orbit transfer theory. The new method is shown to converge to classical impulsive orbit transfer theory in the limit that the duration of the zero-order hold discretization approaches zero and the time horizon extends to infinity. Then the fuel/time optimal control problem is solved using a hybrid approach which uses a linear program to solve the fuel optimization, and a genetic algorithm to find the minimizing time-of-flight. The method developed in this work allows mission planners to determine the feasibility for realistic spacecraft and motion models. Proximity operations for robotic inspection have the potential to aid manned and unmanned systems in space situational awareness and contingency planning in the event of emergency. A potential limiting factor is the large number of constraints imposed on the inspector vehicle due to collision avoidance constraints and limited power and computational resources. We examine this problem and present a solution to the coupled orbit and attitude control problem using model predictive control. This control technique allows state and control constraints to be encoded as a mathematical program which is solved on-line. We present a new thruster constraint which models the minimum-impulse bit as a semi-continuous variable, resulting in a mixed-integer program. The new model, while computationally more expensive, is shown to be more fuel-efficient than a sub-optimal approximation. The result is a fuel efficient, trajectory tracking, model predictive controller with a linear-quadratic attitude regulator which tracks along a pre-computed ``safe'' trajectory in the presence of un-modeled dynamics on a higher fidelity orbital and attitude model.<br>Ph. D.
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Phipps, Warren E. Jr. "Parallelization of the Naval Space Surveillance Center (NAVSPASUR) satellite motion model." Thesis, Monterey, California. Naval Postgraduate School, 1992. http://hdl.handle.net/10945/24001.

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Approved for public release; distribution is unlimited<br>The Naval Space Surveillance Center (NAVSPASUR) uses an analytic satellite motion model based on the Brouwer-Lyddane theory to assist in tracking over 6000 objects in orbit around the earth. The satellite motion model is implemented by a Fortran subroutine, PPT2. Due to the increasing number of objects required to be tracked, NAVSPASUR desires a method to reduce the computation time of this satellite motion model. Parallel computing offers one method to achieve this objective. This thesis investigates the parallel computing potential of the MAVSPASUR model using the Intel iPSC/2 hypercube multi-computer. The thesis developed several parallel algorithms for the NAVSPASUR satellite motion model using the various methods of parallelization, applies these algorithms to the hypercube, and reports on each algorithm's potential reduction in computation time. A diskette containing the Fortran software is available upon request from neta@boris.math.nps.navy.mil.
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Акуленко, Л. Д., Д. Д. Лещенко та Т. А. Козаченко. "Движения твердого тела, близкие к случаю Лагранжа". Thesis, Сумский государственный университет, 2017. http://essuir.sumdu.edu.ua/handle/123456789/65372.

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В работе исследуется возмущенное движение относительно неподвижной точки динамически симметричного тяжелого твердого тела под действием момента сил произвольной природы. Момент силы тяжести не рассматривается как возмущающий момент, а относится к невозмущенному движению, которое представляет собой движение в случае Лагранжа.
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Oumer, Nassir Workicho. "Visual Tracking and Motion Estimation for an On-orbit Servicing of a Satellite." Doctoral thesis, 2016. https://repositorium.ub.uni-osnabrueck.de/handle/urn:nbn:de:gbv:700-2016092815002.

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This thesis addresses visual tracking of a non-cooperative as well as a partially cooperative satellite, to enable close-range rendezvous between a servicer and a target satellite. Visual tracking and estimation of relative motion between a servicer and a target satellite are critical abilities for rendezvous and proximity operation such as repairing and deorbiting. For this purpose, Lidar has been widely employed in cooperative rendezvous and docking missions. Despite its robustness to harsh space illumination, Lidar has high weight and rotating parts and consumes more power, thus undermines the stringent requirements of a satellite design. On the other hand, inexpensive on-board cameras can provide an effective solution, working at a wide range of distances. However, conditions of space lighting are particularly challenging for image based tracking algorithms, because of the direct sunlight exposure, and due to the glossy surface of the satellite that creates strong reflection and image saturation, which leads to difficulties in tracking procedures. In order to address these difficulties, the relevant literature is examined in the fields of computer vision, and satellite rendezvous and docking. Two classes of problems are identified and relevant solutions, implemented on a standard computer are provided. Firstly, in the absence of a geometric model of the satellite, the thesis presents a robust feature-based method with prediction capability in case of insufficient features, relying on a point-wise motion model. Secondly, we employ a robust model-based hierarchical position localization method to handle change of image features along a range of distances, and localize an attitude-controlled (partially cooperative) satellite. Moreover, the thesis presents a pose tracking method addressing ambiguities in edge-matching, and a pose detection algorithm based on appearance model learning. For the validation of the methods, real camera images and ground truth data, generated with a laboratory tet bed similar to space conditions are used. The experimental results indicate that camera based methods provide robust and accurate tracking for the approach of malfunctioning satellites in spite of the difficulties associated with specularities and direct sunlight. Also exceptional lighting conditions associated to the sun angle are discussed, aimed at achieving fully reliable localization system in a certain mission.
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(11014071), Vivek Muralidharan. "Stretching Directions in Cislunar Space: Stationkeeping and an application to Transfer Trajectory Design." Thesis, 2021.

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<div>The orbits of interest for potential missions are stable or nearly stable to maintain long term presence for conducting scientific studies and to reduce the possibility of rapid departure. Near Rectilinear Halo Orbits (NRHOs) offer such stable or nearly stable orbits that are defined as part of the L1 and L2 halo orbit families in the circular restricted three-body problem. Within the Earth-Moon regime, the L1 and L2 NRHOs are proposed as long horizon trajectories for cislunar exploration missions, including NASA's upcoming Gateway mission. These stable or nearly stable orbits do not possess well-distinguished unstable and stable manifold structures. As a consequence, existing tools for stationkeeping and transfer trajectory design that exploit such underlying manifold structures are not reliable for orbits that are linearly stable. The current investigation focuses on leveraging stretching direction as an alternative for visualizing the flow of perturbations in the neighborhood of a reference trajectory. The information supplemented by the stretching directions are utilized to investigate the impact of maneuvers for two contrasting applications; the stationkeeping problem, where the goal is to maintain a spacecraft near a reference trajectory for a long period of time, and the transfer trajectory design application, where rapid departure and/or insertion is of concern.</div><div><br></div><div>Particularly, for the stationkeeping problem, a spacecraft incurs continuous deviations due to unmodeled forces and orbit determination errors in the complex multi-body dynamical regime. The flow dynamics in the region, using stretching directions, are utilized to identify appropriate maneuver and target locations to support a long lasting presence for the spacecraft near the desired path. The investigation reflects the impact of various factors on maneuver cost and boundedness. For orbits that are particularly sensitive to epoch time and possess distinct characteristics in the higher-fidelity ephemeris model compared to their CR3BP counterpart, an additional feedback control is applied for appropriate phasing. The effect of constraining maneuvers in a particular direction is also investigated for the 9:2 synodic resonant southern L2 NRHO, the current baseline for the Gateway mission. The stationkeeping strategy is applied to a range of L1 and L2 NRHOs, and validated in the higher-fidelity ephemeris model.</div><div><br></div><div>For missions with potential human presence, a rapid transfer between orbits of interest is a priority. The magnitude of the state variations along the maximum stretching direction is expected to grow rapidly and, therefore, offers information to depart from the orbit. Similarly, the maximum stretching in reverse time, enables arrival with a minimal maneuver magnitude. The impact of maneuvers in such sensitive directions is investigated. Further, enabling transfer design options to connect between two stable orbits. The transfer design strategy developed in this investigation is not restricted to a particular orbit but applicable to a broad range of stable and nearly stable orbits in the cislunar space, including the Distant Retrograde Orbit (DROs) and the Low Lunar Orbits (LLO) that are considered for potential missions. Examples for transfers linking a southern and a northern NRHO, a southern NRHO to a planar DRO, and a southern NRHO to a planar LLO are demonstrated.</div>
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Books on the topic "Satellite orbital motion model"

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Reilly, Charles H. A satellite system synthesis model for orbital arc allotment optimization. National Aeronautics and Space Administration, Lewis Research Center, 1987.

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Scheeres, Daniel J. Orbital motion in strongly perturbed environments: Applications to asteroid, comet and planetary satellite orbiters. Springer, 2012.

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Danielson, D. A. Satellite motion around an oblate planet: A perturbation solution for all orbital parameters. Naval Postgraduate School, 1993.

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Snider, James Ralph. Satellite motion around an oblate planet: A perturbation solution for all orbital parameters. Naval Postgraduate School, 1989.

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Dilley, A. C. Improved AVHRR data navigation using automated land feature recognition to correct a satellite orbital model. Commonwealth Scientific and Industrial Research Organization, 1994.

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Phipps, Warren E. Paralellization of the Naval Space Surveillance Center (NAVSPASUR) satellite motion model. Naval Postgraduate School, 1992.

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J, Bourassa Roger, Gruenbaum P. E, and Langley Research Center, eds. Operation of the computer model for microenvironment solar exposure. National Aeronautics and Space Administration, Langley Research Center, 1995.

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Scheeres, Daniel J. Orbital Motion in Strongly Perturbed Environments: Applications to Asteroid, Comet and Planetary Satellite Orbiters. Springer Berlin / Heidelberg, 2014.

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Scheeres, Daniel J. Orbital Motion in Strongly Perturbed Environments: Applications to Asteroid, Comet and Planetary Satellite Orbiters. Springer, 2012.

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Hu, Xuhui. Introduction. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198808466.003.0001.

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This chapter firstly introduces the broad theoretical background within which the research carried out in this book is situated. The theoretical aim of this book is to develop a theory of the syntax of events, which is based on the constructivist approach, in particular Borer’s (2005a,b, 2013) Exo-Skeletal (XS) model—part of the broader framework of generative grammar. The empirical scope of this book includes Chinese and English resultatives, applicative constructions, non-canonical object constructions and motion event constructions in Chinese, and the satellite/verb-framed typology. Both synchronic variation and diachronic change are studied. The organization of this book is also outlined.
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Book chapters on the topic "Satellite orbital motion model"

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Kéchichian, Jean Albert. "The Mathematical Models of the Jet Propulsion Laboratory (JPL) Artificial Satellite Analysis Program (ASAP)." In Orbital Relative Motion and Terminal Rendezvous. Springer International Publishing, 2021. http://dx.doi.org/10.1007/978-3-030-64657-8_12.

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Yan, Ye, Xu Huang, and Yueneng Yang. "Dynamical Model of Lorentz-Augmented Orbital Motion." In Dynamics and Control of Lorentz-Augmented Spacecraft Relative Motion. Springer Singapore, 2016. http://dx.doi.org/10.1007/978-981-10-2603-4_2.

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Broucke, R., and A. Konopliv. "Some Models for the Motion of the Co-orbital Satellites of Saturn." In Long-Term Dynamical Behaviour of Natural and Artificial N-Body Systems. Springer Netherlands, 1988. http://dx.doi.org/10.1007/978-94-009-3053-7_12.

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Exertier, P., G. Metris, Y. Boudon, and F. Barlier. "Mean Orbital Motion of Lageos Satellite Derived from Laser Ranging Observations." In Geodesy and Physics of the Earth. Springer Berlin Heidelberg, 1993. http://dx.doi.org/10.1007/978-3-642-78149-0_29.

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Liu, Lin. "Analytical Non-singularity Perturbation Solutions for Extrapolation of Earth’s Satellite Orbital Motion." In Springer Series in Astrophysics and Cosmology. Springer Nature Singapore, 2023. http://dx.doi.org/10.1007/978-981-19-4839-8_4.

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Joshi, Amitabh. "On the nonlinear orbital motion of the driven two-photon Jaynes-Cummings model." In Coherence and Quantum Optics VIII. Springer US, 2003. http://dx.doi.org/10.1007/978-1-4419-8907-9_100.

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Wang, Zhiwen, Hui Xu, Qianxin Wang, and Yilei He. "A Method for Polar Motion Prediction Based on LS Model of Error Compensation." In China Satellite Navigation Conference (CSNC) 2017 Proceedings: Volume III. Springer Singapore, 2017. http://dx.doi.org/10.1007/978-981-10-4594-3_8.

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Kinoshita, Hiroshi. "Motion of the Orbital Plane of a Satellite Due to a Secular Change of the Obliquity of its Mother Planet." In Interactions Between Physics and Dynamics of Solar System Bodies. Springer Netherlands, 1993. http://dx.doi.org/10.1007/978-94-011-1902-3_29.

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Huntley, David, Drew Rotheram-Clarke, Roger MacLeod, Robert Cocking, Jamel Joseph, and Philip LeSueur. "Landslide Monitoring with RADARSAT Constellation Mission InSAR, RPAS-Derived Point-Clouds and RTK-GNSS Time-Series in the Thompson River Valley, British Columbia, Canada." In Progress in Landslide Research and Technology, Volume 2 Issue 1, 2023. Springer Nature Switzerland, 2023. http://dx.doi.org/10.1007/978-3-031-39012-8_19.

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AbstractIn this paper, we evaluate the effectiveness of four land-deformation measurement techniques for monitoring slow-moving landslides along a high-risk section of the national railway corridor traversing the Thompson River valley, British Columbia, Canada. The geomorphically active North Slide acts as an ideal field laboratory for testing and evaluating novel monitoring techniques and methods. We compare differential processing of Structure from Motion (SfM) products such as point-cloud elevation models and orthophotos derived from Remotely Piloted Aircraft Systems (RPAS), along with satellite based Interferometric Synthetic Aperture Radar (InSAR) deformation measurements derived from RADARSAT Constellation Mission (RCM). These results are ground-truthed with periodic real-time kinematic (RTK) global navigation satellite system (GNSS) measurements. We evaluate point-cloud comparison techniques, including the multi-scale model-to-model cloud comparison (M3C2) algorithm and digital ortho image correlation techniques. Multi-temporal RCM InSAR deformation measurements are processed using a semi-automated processing system for interferogram generation and unwrapping. Manual processing of small baseline subsets (SBAS) leads to the recovery of 1-dimensional line-of-sight (LoS) and 2-dimensional deformation measurements. Lastly, we discuss the strengths and limitations of these techniques, considerations for interpreting their outputs, and considerations for direct comparisons between InSAR, RPAS and RTK-GNSS deformation measurements.
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Guerrini, Federica. "Data-Informed Models for the Coupled Dispersal of Microplastics and Related Pollutants Applied to the Mediterranean Sea." In Special Topics in Information Technology. Springer International Publishing, 2022. http://dx.doi.org/10.1007/978-3-031-15374-7_1.

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AbstractMicroplastic pollution is a ubiquitous environmental threat, in particular to the oceans. In the marine environment, microplastics are not just passively transported by sea currents, but often get contaminated with organic pollutants during the journey. The uptake of chemicals onto microplastics can worsen the adverse effects of microplastics to marine organisms; however, investigation on this urgent phenomenon is hampered by the impossibility of monitoring and tracking such small plastic fragments during their motion at sea. This work aims at addressing the need for an effective modelling of the advection–diffusion processes jointly involving microplastics and the pollutants they carry to further our understanding of their spatiotemporal patterns and ecological impacts, focusing on the Mediterranean Sea. Here we present the conceptual design, methodological settings, and modelling results of a novel, data-informed 2D Lagrangian–Eulerian modelling framework that simultaneously describes (i) the Lagrangian dispersal of microplastic on the sea surface, (ii) the Eulerian advection–diffusion of selected organic contaminants, and (iii) the gradient-driven chemical exchanges between microplastic particles and chemical pollutants in the marine environment in a simple, yet comprehensive way. Crucial to the realism of our model is exploiting the wide variety and abundance of data linked with drivers of Mediterranean marine pollution by microplastics and chemicals, ranging from national censuses to satellite data of surface water runoff and GPS ship tracking, other than the use of oceanographic reanalyses to inform microplastics’ motion at sea. The results of our method applied to a multi-year simulation contribute to a first basin-wide assessment of the role of microplastics as a vehicle of other pollutants of concern in the marine environment. The framework proposed here is intended as a flexible tool to help advance knowledge towards a comprehensive description of the multifaceted threat of marine plastic pollution and an informed support to targeted mitigation policies.
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Conference papers on the topic "Satellite orbital motion model"

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Kim, Junsik, Yuna Choi, Youngjin Choi, et al. "Axis Kinematics Algorithm for Satellite Manipulator System in Orbital Motion." In 2024 International Conference on Space Robotics (iSpaRo). IEEE, 2024. http://dx.doi.org/10.1109/isparo60631.2024.10687540.

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Lv, Chongyu, Sheng Fang, Boyu Hua, et al. "Buoy Loss Model for Satellite-to-sea Communication Cooperating 6D Motion." In 2024 Photonics & Electromagnetics Research Symposium (PIERS). IEEE, 2024. http://dx.doi.org/10.1109/piers62282.2024.10618358.

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Alesia Herasimenka, Miss, Ariadna Farrés, and Lamberto Dell'Elce. "Station-keeping under conical constraint on the control force." In ESA 12th International Conference on Guidance Navigation and Control and 9th International Conference on Astrodynamics Tools and Techniques. ESA, 2023. http://dx.doi.org/10.5270/esa-gnc-icatt-2023-082.

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Due to specific mission goals, many satellites are subject to cone constraints on the thrust direction. For example, James Webb Space Telescope, launched on December 25, 2021 toward a Halo orbit around the Sun-Earth L2 libration point, has a thermal shield that must prevent the telescope and other instruments from overheating [1]. Therefore, it is constrained to always keep its attitude such that the angle between the normal to the shield and the Sun direction is smaller than 53 deg. It results in conical constraints for the propulsion directions. Using chemical propulsion to perform small impulsive corrections of the trajectory or a low-thrust satellite with very specific constraints on the control does not always allow to do any desirable maneuver, as we showed in [2], where the controllability of non-ideal solar sails in orbit about a planet was investigated. In [2], we considered elliptic Keplerian orbits, and we formulated a convex optimization problem aimed at assessing whether some functions of the integrals of motion could not be decreased after one orbital period. Existence of such functions implies that there is a half-space of the neighborhood orbit's coordinates (orbital elements) where motion is locally forbidden [3]. In that paper, we strongly relied on the super-integrability of the Kepler problem. Here, we extend the methodology to infer local controllability of station-keeping satellites for any periodic orbit, regardless the dynamical system at hand. Given the projection of the nominal orbit on a surface of section, the methodology aims at verifying if a half space of such projection exists where the motion is forbidden after one orbital period. Variation of parameters is used to achieve a convex optimization problem that investigates the existence of obstructions to variations of local integrals of motion. Conical constraints are enforced by leveraging on the formalism of positive polynomials postulated by Nesterov [4], so that a finite-dimensional formulation of the convex program is achieved. Halo orbit in the CRTBP is eventually considered in the case study, but we emphasize again that the methodology is developed for a generic locally-integrable system. We compare the aforedescribed methodology with the results achieved in [5], where the authors looked at the controllability and the impact of limitations of the thrust direction on the station-keeping from a dynamical point of view. They use the Floquet Mode reference frame to describe the motion of the satellite in a close proximity to the orbit, and study the cost of station-keeping by projecting the thrust direction on the saddle plane. The minimum requirement that we propose can be used for a design of space missions around any periodic orbit for satellites that have specific constraints on the thrust directions. It can be applied to a low-thrust satellite or even those with chemical propulsion under condition of using small impulses, so that the linearization of the dynamics holds. [1] J. Petersen, “L2 Station Keeping Maneuver Strategy For The James Webb Space Telescope,” AIAA/AAS Astrodynamics Specialist Conference, American Institute of Aeronautics and Astronautics, 2019. [2] A. Herasimenka, L. Dell’Elce, J.-B. Caillau, and J.-B. Pomet, “Controllability Properties of Solar Sails,” Journal of Guidance, Control, and Dynamics, 2022. in press. [3] J.-B. Caillau, L. Dell’Elce, A. Herasimenka, and J.-B. Pomet, “On the Controllability of Nonlinear Systems with a Periodic Drift,” 2022. HAL preprint no. 03779482. [4] Y. Nesterov, “Squared Functional Systems and Optimization Problems,” High Performance Optimization (P. M. Pardalos, D. Hearn, H. Frenk, K. Roos, T. Terlaky, and S. Zhang, eds.), Vol. 33, pp. 405–440, Boston, MA: Springer US, 2000. Series Title: Applied Optimization, 10.1007/978-1-4757-3216-0 17. [5] A. Farres, C. Gao, J. J. Masdemont, G. Gomez, D. C. Folta, and C. Webster, “Geometrical Analysis of Station-Keeping Strategies About Libration Point Orbits,” Journal of Guidance, Control, and Dynamics, Vol. 45, June 2022, https://arc.aiaa.org/doi/10.2514/1.G006014.
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Mankala, Kalyan K., and Sunil K. Agrawal. "Dynamic Modeling and Simulation of Impact in Tether Net/Gripper Systems." In ASME 2003 International Design Engineering Technical Conferences and Computers and Information in Engineering Conference. ASMEDC, 2003. http://dx.doi.org/10.1115/detc2003/vib-48505.

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The objective of this paper is to study the dynamic modeling and simulation of a tether-net/gripper system during an impact, while it is being deployed or retrieved by a winch on a satellite orbiting around earth. We stick to Tether-Net system but the analysis is applicable to Tether-Gripper systems too. We assume that the net is deployed from the satellite in orbit and the motion is restricted to the orbital plane. This net captures a second satellite and tows it. The motion of a tether-net system can be broken down into the following phases: (i) Phase 1: Net is shot out from the satellite with the tether completely slack, (ii) Phase 2: Net comes to a location where the tether is taut while the drum on the orbiter is locked, (iii) Phase 3: Drum is unlocked and the net moves with the tether, (iv) Phase 4: Net captures a body. The continua (tether) is modeled using mode functions and coordinates. The theory of impulse and momentum can be used to model Phases 1, 2, and 4 of motion of the tether-net system. The dynamics of the motion of the system in phase 3 is characterized by differential and algebraic equations (DAEs). Matlab ODE solvers were used to solve these DAEs.
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Mankala, Kalyan K., and Sunil K. Agrawal. "Dynamic Modeling and Simulation of Satellite Tethered Systems." In ASME 2003 International Design Engineering Technical Conferences and Computers and Information in Engineering Conference. ASMEDC, 2003. http://dx.doi.org/10.1115/detc2003/vib-48344.

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The objective of this paper is to study the dynamic simulation of a tether as it is deployed or retrieved by a winch on a satellite orbiting around earth. In an effort to understand the problem incrementally, the following three models were developed: (a) Model 1: A tether with constant length moves on earth in the plane of constant gravity; (b) Model 2: A tether is deployed from a drum on earth in the plane of constant gravity, i.e., length of the cable changes during deployment; (c) Model 3: A tether is deployed from a drum on an orbiting satellite. These models have been chosen to bring different aspects as well as levels of difficulty in the analysis. For example, in Model 1, the length of cable is fixed and the gravity direction is constant during motion. The equations of motion for this model are derived using Newton’s laws and Hamilton’s principle to show the equivalence of the two methods. In Model 2, free length of the cable changes during deployment. The changing length of the cable introduces coupled nonlinearities into the motion. Model 3 includes the orbital effect on the motion of deployed cable. Each of these three dynamic models characterized by partial differential equations are first converted to a finite number of ordinary differential equations using Ritz’s procedure and are then numerically integrated using Matlab ODE solvers.
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Aliberti, Stefano, Marco B. Quadrelli, and Marcello Romano. "Dynamics and Aerodynamic Control of a Cross-Track Tether Satellite System." In ESA 12th International Conference on Guidance Navigation and Control and 9th International Conference on Astrodynamics Tools and Techniques. ESA, 2023. http://dx.doi.org/10.5270/esa-gnc-icatt-2023-098.

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The objective of this paper is to present and analyze the dynamics and control strategy of a novel type of formation flight architecture, that could enable unprecedented space mission capabilities. In particular we propose and study a tether satellite system composed by two or more satellites, flying in LEO, connected by a linear tether. That tether is maintained in tension along the cross-track direction, with respect to the orbit, i.e., perpendicular to the motion and radial directions, by exploiting the aerodynamic lift acting upon the suitably oriented satellites. Possible applications of this formation are related, in particular, to remote sensing. To carry out the study, a three-dimensional multibody model was developed, introducing the equations of relative dynamics centered in an orbiting reference frame. To simulate the conditions of low Earth orbit, several mathematical models taken from the literature were used, in order to include the Earth’s gravitational potential up to fourth order, solar pressure, third-body perturbations, atmospheric drag and the behavior of aerodynamic surfaces in a free molecular flow. By utilizing this model and verifying that this configuration is intrinsically unstable, it was concluded that the system needs continuous control to be stabilized. As a result, the model of the dynamics was linearized and an optimal LQR controller was introduced to calculate the force required to hold the system in place. Once the linear control law was validated by simulating its application on the full system model, aerodynamic surfaces were next introduced in order to generate the force required for control by taking advantage of the rarefied atmosphere of low Earth orbit. The proposed control strategy is tested by extensive numerical simulations. Finally, the proposed aerodynamic stabilization approach to continuously maintain a linear tether satellite system along the cross-track direction was compared to a gyroscopic stabilization alternative strategy. This strategy consists of putting the system into rotation in a direction perpendicular to the cross-track direction. The centrifugal force generated by the rotation stabilizes the system, maintaining constant oscillations in the cross-track direction throughout the orbit. Both cases have been analyzed as the size of the system and the number of satellites change.
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Terui, Fuyuto, Heihachiro Kamimura, and Shin' ichiro Nishida. "Motion Estimation to a Failed Satellite on Orbit using Stereo Vision and 3D Model Matching." In 2006 9th International Conference on Control, Automation, Robotics and Vision. IEEE, 2006. http://dx.doi.org/10.1109/icarcv.2006.345305.

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Babanin, Alexander V. "Swell Attenuation due to Wave-Induced Turbulence." In ASME 2012 31st International Conference on Ocean, Offshore and Arctic Engineering. American Society of Mechanical Engineers, 2012. http://dx.doi.org/10.1115/omae2012-83706.

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In the paper, we will discuss two separate, but connected issues: wave-turbulence interactions, and estimates of swell attenuation due to such turbulence. Theoreticaly, potential waves cannot generate the vortex motion, but the scale considerations indicate that if the steepness of waves is not too small, the Reynolds number can exceed the critical values. This means that in presence of initial non-potential disturbances the orbital velocities can generate the vortex motion and turbulence. This problem was investigated by laboratory means, numerical simulations and field observations. As a sink of wave energy, such dissipation is small in presence of wave breaking, but is essential for swell. Swell prediction by spectral wave models is often poor, but is important for offshore and maritime industry. Based on the research of wave-induced turbulence, new swell-dissipation function is proposed. It agrees well with satellite observations of long-distance swell propagation and is being employed and tested in spectral wave models.
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Casu, Davide, Vincent Dubanchet, Hervé Renault, Anthea Comellini, and Pierre Dandré. "EROSS+ Phase A/B1 Guidance, Navigation and Control design for In-Orbit Servicing." In ESA 12th International Conference on Guidance Navigation and Control and 9th International Conference on Astrodynamics Tools and Techniques. ESA, 2023. http://dx.doi.org/10.5270/esa-gnc-icatt-2023-036.

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The H2020 project “EROSS+ Phase A/B1” standing for “European Robotic Orbital Support Services” has been over 2021-2023 to mature the future robotic servicing missions with a highly-autonomous and coupled Guidance, Navigation and Control (GNC) architecture for both a satellite platform and its embedded robotic arm. This project is built upon the previous developments of the Operational Grants led by the Strategic Research Cluster in Space Robotics funded by the European Commission since 2016. More specifically, EROSS+ project aims at deriving a system design of a robotic Servicer approaching, capturing and servicing a Client satellite. It thus integrates and demonstrates the key European robotic building blocks by demonstrating their performances from Model in the Loop (MIL) tests to Hardware in the Loop (HIL) experiments. The main use-case of EROSS+ project is to demonstrate the capability of a Servicer spacecraft to perform medium and close-range rendezvous, before capturing and manipulating a Client satellite with a high degree of autonomy. The client satellite is considered collaborative and prepared for servicing operations such as refuelling and payload replacement. EROSS+ timeline is based on four main steps covering the approach with an autonomous visual-based navigation using advanced processing and filtering techniques; the capture using state-of-the-art compliance control techniques to synchronize the robotic arm and its platform; the mating of the two spacecrafts through a dedicated interface for refuelling; and then the robotic exchange of a replacement payload designed with standard interfaces. The goal of this article is to present the work done in EROSS+ Phase A/B1 aiming at deriving a versatile GNC architecture for multi-orbit purposes LEO and GEO minimizing delta-design impact. Initially, we will present an overview of the main design drivers and requirements, both in terms of mission constraint (e.g., ground station visibility for communication and monitoring of critical operations, observability constraints) and safety requirements (e.g. exclusion zones, approach corridors, and GO/NO-GO decision at predefined hold points). In fact, the RDV strategy proposed has to be compliant to the ESA Safe Proximity Operation guidelines and the French Space Act (“Lois des Operations Spatiales”). A high level description of the CONcept of OPerationS (CONOPS) will be provided, focusing on the strategy from Phasing, Homing, Closing, Inspection, Approach and Capture. The RDV mission will be divided in a long-range phase with absolute to relative navigation synergy and full autonomous handover, and an autonomous but supervised safe short-range phase. A description of the mission timeline will follow, taking into account the synchronization of visibility windows for data exchange with Ground (operational procedures, checks and TC GO/NO-GO, monitoring, data downloading/uploading), the execution of maneuvers from main boost to correction maneuvers, and navigation observability constraints for vision, based navigation (e.g., Sun Phase Angle and eclipses). Short range maneuvers from fly-around, inspection and forced motions along predefined corridors will lead the Servicer to the capture-point conditions, where the robotic arm will initiate robotic capture and mating. Then, we will focus on the On-Board Autonomy layer and high level FDIR strategy, complying with the safety guidelines of uncrewed missions but still considering the high criticality of the RDV operations (with the constraint of avoiding collisions while ensuring a high probability of completing the mission -without executing too many cost impacting Collision Avoidance Maneuvers). A special attention is given on how safety is addressed and ensured in the GNC design, and verified during the Validation &amp; Verification (V&amp;V) process (safety by design is ensured when possible -i.e. passive safe orbits design-), and how early safety and FDIR analyses impact the overall architecture and design choices. Subsequently, we will detail the GNC operational modes and phases to ensure the In-Orbit Servicing mission, firstly describing the high level architecture, which is oriented on the operational modes and the Hardware Matrix (i.e. classical modes such as Stand-By Mode (SBM), Safe Hold Mode (SHM), Nominal Mode (NOM), Orbit Control Mode (OCM) for absolute navigation, will be presented along with RDV &amp; capture modes and Collision Avoidance Mode), and secondly focusing on the mid-level layer, which consists in GNC phases (e.g., Station-Keeping (SK), 6 Degree-Of-Freedom forced motion, and others). The GNC architecture will have to take into account the typical challenges of RDV &amp; capture in terms of HW (i.e., the presence of optical sensors for vision based navigation and image processing, the robotic arm for capture, and so on). Then, an overview of the main functions of Guidance (e.g., computation of several maneuvers from long range to inspection, fly-around, R-Bar and V-bar forced motions), Navigation (with focus on multiple sensors data fusion) and Control (e.g., open loop, 6DOF Robust control, robotic arm and platform coordinated control) will be provided. Finally, we will present an brief overview of the GNC workflow -from design to Validation and Verification (V&amp;V)- executed following the Agile philosophy to be pursued along the following EROSS In-Orbit Demonstration (IOD) program. The V&amp;V process is allowing fast prototyping from building blocks development to flight software, thanks to the autocode framework and early integration of the GNC software in representative space hardware, to asses required computational budgets and confirm early preliminary algorithms profiling. Early testing of several hardware elements has taken place during the Hardware-In-the-Loop testing (e.g. vision systems capability assessments in robotic test benches) to corroborate Processor-In-the-Loop, Model-In-the-Loop, and Software-In-the-Loop tests, from open-loop simulations to full GNC closed-loop ones. The core GNC software is claimed to be at TRL5 at the end of EROSS+ Phase B1. EROSS+ project has been co-funded by European Union’s Horizon 2020 research and innovation program under grant agreement N°101004346 and is part of the Strategic Research Cluster on Space Robotics Technologies as Operational Grant n°12. Thales Alenia Space has led this project in collaboration with DLR, GMV, SINTEF AS, and PIAP Space.
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10

Lampariello, Roberto, and Gerhard Hirzinger. "Modeling and Experimental Design for the On-Orbit Inertial Parameter Identification of Free-Flying Space Robots." In ASME 2005 International Design Engineering Technical Conferences and Computers and Information in Engineering Conference. ASMEDC, 2005. http://dx.doi.org/10.1115/detc2005-85242.

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A method is proposed for the identification of the inertial parameters of a free-flying robot directly in orbit, using accelerometers. This can serve to improve the path planning and tracking capabilities of the robot, as well as its efficiency in energy consumption. The method is applied to the identification of the base body and of the load on the end-effector, giving emphasis to the experimental design. The problem of the identification of the full system is also addressed in its theoretical aspects. The experience from the Getex Dynamic Motion experiments performed on the ETS-VII satellite have allowed to determine a most suitable model for the identification.
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Reports on the topic "Satellite orbital motion model"

1

Danielson, D. A., G. E. Latta, C. P. Sagovac, S. D. Krambeck, and J. R. Snider. Satellite Motion Around an Oblate Planet: A Perturbation Solution for All Orbital Parameters. Defense Technical Information Center, 1993. http://dx.doi.org/10.21236/ada265779.

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2

Phipps, Jr, Neta Warren E., Danielson Beny, and D. A. Parallelization of the Naval Space Surveillance Satellite Motion Model. Defense Technical Information Center, 1993. http://dx.doi.org/10.21236/ada531142.

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3

Beason, Scott, Taylor Kenyon, Robert Jost, and Laurent Walker. Changes in glacier extents and estimated changes in glacial volume at Mount Rainier National Park, Washington, USA from 1896 to 2021. National Park Service, 2023. http://dx.doi.org/10.36967/2299328.

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Surface area of glaciers and perennial snow within Mount Rainier National Park were delineated based on 2021 aerial Structure-from-Motion (SfM) and satellite imagery to document changes to glaciers over the last 125 years. These extents were compared with previously completed databases from 1896, 1913, 1971, 1994, 2009, and 2015. In addition to the glacial features mapped at the Park, any snow patches noted in satellite- and fixed-wing- acquired aerial images in September 2021 were mapped as perennial snowfields. In 2021, Mount Rainier National Park contained a total of 28 named glaciers which covered a total of 75.496 ± 4.109 km2 (29.149 ± 1.587 mi2). Perennial snowfields added another 1.938 ± 0.112 km2 (0.748 ± 0.043 mi2), bringing the total perennial snow and glacier cover within the Park in 2021 to 77.434 ± 4.221 km2 (29.897 ± 1.630 mi2). The largest glacier at Mount Rainier was the Emmons Glacier, which encompasses 10.959 ± 0.575 km2 (4.231 ± 0.222 mi2). The change in glacial area from 1896 to 2021 was -53.812 km2 (-20.777 mi2), a total reduction of 41.6%. This corresponds to an average rate of -0.430 km2 per year (-0.166 mi2 × yr-1) during the 125 year period. Recent changes (between the 6-year period of 2015 to 2021) showed a reduction of 3.262 km2 (-1.260 mi2) of glacial area, or a 4.14% reduction at a rate of -0.544 km2 per year ( 0.210 mi2 × yr-1). This rate is 2.23 times that estimated in 2015 (2009-2015) of -0.244 km2 per year (-0.094 mi2 × yr-1). Changes in ice volume at Mount Rainier and estimates of total volumes were calculated for 1896, 1913, 1971, 1994, 2009, 2015, and 2021. Volume change between 1971 and 2007/8 was -0.65 km3 ( 0.16 mi3; Sisson et al., 2011). We used the 2007/8 LiDAR digital elevation model and our 2021 SfM digital surface model to estimate a further loss of -0.404 km3 (-0.097 mi3). In the 50-year period between 1971 and 2021, the glaciers and perennial snowfields of Mount Rainier lost a total of -1.058 km3 (-0.254 mi3) at a rate of -0.021 km3 per year (-0.005 mi3 × yr-1). The calculation of the total volume of the glaciers during various glacier extent inventories at Mount Rainier is not straightforward and various methods are explored in this paper. Using back calculated scaling parameters derived from a single volume measurement in 1971 and estimates completed by other authors, we have developed an estimate of glacial mass during the last 125-years at Mount Rainier that mostly agree with volumetric changes observed in the last 50 years. Because of the high uncertainty with these methods, a relatively modest 35% error is chosen. In 2021, Mount Rainier’s 28 glaciers contain about 3.516 ± 1.231 km3 (0.844 ± 0.295 mi3) of glacial ice, snow, and firn. The change in glacial mass over the 125-year period from 1896 to 2021 was 3.742 km3 (-0.898 mi3), a total reduction of 51.6%, at an average rate of -0.030 km3 per year ( 0.007 mi3 × yr-1). Volume change over the 6-year period of 2015 to 2021 was 0.175 km3 (-0.042 mi3), or a 4.75% reduction, at a rate of -0.029 km3 per year (-0.007 mi3 × yr-1). This survey officially removes one glacier from the Park’s inventory and highlights several other glaciers in a critical state. The Stevens Glacier, an offshoot of the Paradise Glacier on the Park’s south face, was removed due to its lack of features indicating flow, and therefore is no longer a glacier but instead a perennial snowfield. Two other south facing glaciers – the Pyramid and Van Trump glaciers – are in serious peril. In the six-year period between 2015 and 2021, these two glaciers lost 32.9% and 33.6% of their area and 42.0% and 42.9% of their volume, respectively. These glaciers are also becoming exceedingly fragmented and no longer possess what can be called a main body of ice. Continued losses will quickly lead to the demise of these glaciers in the coming decades. Overall, the glaciers on the south face of the mountain have been rapidly shrinking over the last 125 years. Our data shows a continuation of gradual yet accelerating loss of glacial ice at Mount Rainier, resulting in significant changes in regional ice volume over the last century. The long-term impacts of this loss will be widespread and impact many facets of the Park ecosystem. Additionally, rapidly retreating south-facing glaciers are exposing large areas of loose sediment that can be mobilized to proglacial rivers during rainstorms, outburst floods, and debris flows. Regional climate change is affecting all glaciers at Mount Rainier, but especially those smaller cirque glaciers and discontinuous glaciers on the south side of the volcano. If the regional climate trend continues, further loss in glacial area and volume parkwide is anticipated, as well as the complete loss of small glaciers at lower elevations with surface areas less than 0.2 km2 (0.08 mi2) in the next few decades.
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